IP Library Granted Patent US 7,315,426
Granted Patent B2
US 7,315,426 · App. 11/001,154 · Granted Jan 1, 2008

Metallic nano-optic lenses and beam shaping devices

Assignee: University of Pittsburgh
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Quick Facts
Patent No.
US 7,315,426
App. No.
11/001,154
Granted
Jan 1, 2008
Kind
B2
Abstract

A nano-optic device comprises a plurality of subwavelength apertures in a metal film or between metal islands. The device is adapted to shape a radiation beam transmitted there through. For example, beam shaping includes at least one of beam focusing, beam bending and beam collimating.

Claims (51)

1. A nano-optic device comprising a plurality of subwavelength apertures in a metal film or between metal islands, wherein the device is adapted to shape a radiation beam transmitted there through and wherein:

each aperture has a width that is less than a first peak wavelength of incident radiation to be provided onto the film or islands; and

the metal film or islands are configured such that the incident radiation is resonant with at least one plasmon mode on the metal film or metal islands, thereby enhancing transmission of radiation having at least one second peak wavelength through the apertures.

2. The device of claim 1 , wherein shaping the radiation beam comprises at least one of beam focusing, beam bending and beam collimating.

3. The device of claim 1 , wherein the device comprises a lens which is adapted to focus the radiation beam to a spot that is the same as or smaller than a peak wavelength of the radiation beam.

4. The device of claim 3 , wherein the spot size ranges from 10 nm to 800 nm.

5. The device of claim 3 , wherein the lens comprises a metal film having a convex profile such that the apertures have a different depth in a half elliptical profile.

6. The device of claim 3 , wherein the lens comprises a flat metal film containing the apertures and a dielectric lens mounted thereon.

7. The device of claim 1 , wherein the device is a beam bending device comprising a metal film containing different transparent refractive index materials in different apertures, above different apertures or in and above different apertures.

8. The device of claim 1 , wherein the device is a beam bending device comprising a metal film containing, or metal islands separated by, apertures of different width.

9. The device of claim 1 , wherein the device further comprises at least one of a spatial, wavelength and polarization filter.

10. The device of claim 1 , wherein the device is used together with at least one of a spatial, wavelength and polarization filter.

11. The device of claim 1 , wherein each aperture serves as a dipole source radiating optical power at an exit surface of the metal film or islands.

12. The device of claim 11 , wherein the dipole elements are designed to have a predetermined phase relationship among them controlled by at least one of a path length difference and an effective index difference in the aperture regions.

13. The device of claim 1 , wherein the aperture width is between 15 nm and 700 nm.

14. A nano-optic device comprising a plurality of subwavelength apertures in a metal film or between metal islands, wherein the device is adapted to shape a radiation beam transmitted there through and wherein:

the device comprises a lens which is adapted to focus the radiation beam to a spot that is the same as or smaller than a peak wavelength of the radiation beam; and

the lens comprises:

i) a metal film or metal islands having a convex profile such that the apertures have a different depth in a half elliptical profile; or

ii) a dielectric lens mounted on a flat metal film containing the apertures or on flat metal islands separated by the apertures.

15. The device of claim 14 , wherein the spot size ranges from 10 nm to 800 nm and the aperture width is between 15 nm and 700 nm.

16. The device of claim 14 , wherein:

each aperture has a width that is less than a first peak wavelength of incident radiation to be provided onto the film or islands; and

the metal film or islands are configured such that the incident radiation is resonant with at least one plasmon mode on the metal film or metal islands, thereby enhancing transmission of radiation having at least one second peak wavelength through the apertures.

17. The device of claim 14 , wherein the device further comprises at least one of a spatial, wavelength and polarization filter or the device is used together with at least one of a spatial, wavelength and polarization filter.

18. The device of claim 14 , wherein:

each aperture serves as a dipole source radiating optical power at an exit surface of the metal film or islands; and

the dipole elements are designed to have a predetermined phase relationship among them controlled by at least one of a path length difference and an effective index difference in the aperture regions.

19. The device of claim 14 , wherein the lens comprises the metal film having the convex profile such that the apertures have the different depth in the half elliptical profile.

20. The device of claim 14 , wherein the lens comprises the metal islands having the convex profile such that the apertures have the different depth in the half elliptical profile.

21. The device of claim 14 , wherein the lens comprises the dielectric lens mounted on the flat metal film containing the apertures.

22. The device of claim 14 , wherein the lens comprises the dielectric lens mounted on the flat metal islands separated by the apertures.

23. A nano-optic device comprising a plurality of subwavelength apertures in a metal film or between metal islands, wherein the device is adapted to shape a radiation beam transmitted there through and the device comprises a beam bending device wherein:

i) the metal film contains apertures of different width; or

ii) the metal islands are separated by apertures of different width; or

iii) different transparent refractive index materials are located in different apertures, above different apertures or in and above different apertures.

24. The device of claim 23 , wherein the aperture width is between 15 nm and 700 nm.

25. The device of claim 23 , wherein:

each aperture has a width that is less than a first peak wavelength of incident radiation to be provided onto the film or islands; and

the metal film or islands are configured such that the incident radiation is resonant with at least one plasmon mode on the metal film or metal islands, thereby enhancing transmission of radiation having at least one second peak wavelength through the apertures.

26. The device of claim 23 , wherein the device further comprises at least one of a spatial, wavelength and polarization filter or the device is used together with at least one of a spatial, wavelength and polarization filter.

27. The device of claim 23 , wherein:

each aperture serves as a dipole source radiating optical power at an exit surface of the metal film or islands; and

the dipole elements are designed to have a predetermined phase relationship among them controlled by at least one of a path length difference and an effective index difference in the aperture regions.

28. The device of claim 23 , wherein the device comprises the metal film containing apertures of different width.

29. The device of claim 23 , wherein the device comprises the metal islands separated by apertures of different width.

30. The device of claim 23 , wherein the device comprises different transparent refractive index materials located in different apertures, above different apertures, or in and above different apertures.

31. A nano-optic device comprising a plurality of subwavelength apertures in a flat metal film or between metal islands, wherein the device is adapted to shape a radiation beam transmitted there through and wherein the device further comprises at least one of a spatial, wavelength and polarization filter.

32. A nano-optic device comprising a plurality of subwavelength apertures in a flat metal film or between metal islands, wherein the device is adapted to shape a radiation beam transmitted there through and wherein:

each aperture serves as a dipole source radiating optical power at an exit surface of the metal film or islands; and

the dipole elements are designed to have a predetermined phase relationship among them controlled by at least one of a path length difference and an effective index difference in the aperture regions.

Assignments (2)
CONFIRMATORY LICENSE Recorded Aug 12, 2008
From: PITTSBURGH, UNIVERSITY OF
To: NAVY, SECRETARY OF THE, UNITED STATES OF AMERICA
Reel/Frame 021388/0246 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 1, 2005
From: KIM, HONG KOO; SUN, ZHIJUN; CAPELLI, CHRISTOPHER C.
To: PITTSBURGH, UNIVERSITY OF
Reel/Frame 016441/0093 →
Continuity (2)
Provisional Application 6052699800 · Dec 5, 2003
Related Publication 20050161589A1 · Jul 28, 2005